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000588138 0247_ $$2ISSN$$a0031-9163
000588138 0247_ $$2ISSN$$a0370-2693
000588138 0247_ $$2ISSN$$a1873-2445
000588138 0247_ $$2arXiv$$aarXiv:2301.10731
000588138 0247_ $$2datacite_doi$$a10.3204/PUBDB-2023-04754
000588138 037__ $$aPUBDB-2023-04754
000588138 041__ $$aEnglish
000588138 082__ $$a530
000588138 088__ $$2arXiv$$aarXiv:2301.10731
000588138 088__ $$2CERN$$aCERN-EP-2022-289
000588138 1001_ $$0P:(DE-HGF)0$$aATLAS Collaboration$$b0$$eCollaboration author
000588138 245__ $$aCombination of searches for invisible decays of the Higgs boson using 139 fb−1 of proton-proton collision data at s=13 TeV collected with the ATLAS experiment
000588138 260__ $$c2023
000588138 3367_ $$0PUB:(DE-HGF)25$$2PUB:(DE-HGF)$$aPreprint$$bpreprint$$mpreprint$$s1691154337_1266264
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000588138 3367_ $$2BibTeX$$aARTICLE
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000588138 500__ $$aPhys. Lett. B 842 (2023) 137963. All figures including auxiliary figures are available at https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2021-05
000588138 520__ $$aMany extensions of the Standard Model predict the production of dark matter particles at the LHC. Sufficiently light dark matter particles may be produced in decays of the Higgs boson that would appear invisible to the detector. This Letter presents a statistical combination of searches for H→invisible decays where multiple production modes of the Standard Model Higgs boson are considered. These searches are performed with the ATLAS detector using 139 fb−1 of proton–proton collisions at a centre–of–mass energy of Image 1 at the LHC. In combination with the results at Image 2 and Image 3, an upper limit on the H→invisible branching ratio of 0.107 (0.077) at the 95% confidence level is observed (expected). These results are also interpreted in the context of models where the 125 GeV Higgs boson acts as a portal to dark matter, and limits are set on the scattering cross-section of weakly interacting massive particles and nucleons.
000588138 536__ $$0G:(DE-HGF)POF4-611$$a611 - Fundamental Particles and Forces (POF4-611)$$cPOF4-611$$fPOF IV$$x0
000588138 588__ $$aDataset connected to CrossRef, INSPIRE, Journals: bib-pubdb1.desy.de
000588138 650_7 $$2INSPIRE$$ap p: scattering
000588138 650_7 $$2INSPIRE$$ap p: colliding beams
000588138 650_7 $$2INSPIRE$$aHiggs particle: hadroproduction
000588138 650_7 $$2INSPIRE$$adark matter: pair production
000588138 650_7 $$2INSPIRE$$aHiggs particle: invisible decay
000588138 650_7 $$2INSPIRE$$aHiggs particle: decay modes
000588138 650_7 $$2INSPIRE$$aCERN LHC Coll
000588138 650_7 $$2INSPIRE$$aATLAS
000588138 650_7 $$2INSPIRE$$aHiggs particle: branching ratio
000588138 650_7 $$2INSPIRE$$abranching ratio: upper limit
000588138 650_7 $$2INSPIRE$$aWIMP nucleon: scattering
000588138 650_7 $$2INSPIRE$$aWIMP nucleon: cross section
000588138 650_7 $$2INSPIRE$$achannel cross section: upper limit
000588138 650_7 $$2INSPIRE$$amultiple production
000588138 650_7 $$2INSPIRE$$aWIMP: dark matter
000588138 650_7 $$2INSPIRE$$aWIMP: mass
000588138 650_7 $$2INSPIRE$$astatistical
000588138 650_7 $$2INSPIRE$$aexperimental results
000588138 650_7 $$2INSPIRE$$a7000 GeV-cms
000588138 650_7 $$2INSPIRE$$a8000 GeV-cms
000588138 650_7 $$2INSPIRE$$a13000 GeV-cms
000588138 693__ $$0EXP:(DE-H253)LHC-Exp-ATLAS-20150101$$1EXP:(DE-588)4398783-7$$5EXP:(DE-H253)LHC-Exp-ATLAS-20150101$$aLHC$$eLHC: ATLAS$$x0
000588138 8564_ $$uhttps://bib-pubdb1.desy.de/record/588138/files/230804_2301.10731.pdf$$yOpenAccess
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000588138 9101_ $$0I:(DE-588b)2008985-5$$6P:(DE-HGF)0$$aDeutsches Elektronen-Synchrotron$$b0$$kDESY
000588138 9131_ $$0G:(DE-HGF)POF4-611$$1G:(DE-HGF)POF4-610$$2G:(DE-HGF)POF4-600$$3G:(DE-HGF)POF4$$4G:(DE-HGF)POF$$aDE-HGF$$bForschungsbereich Materie$$lMatter and the Universe$$vFundamental Particles and Forces$$x0
000588138 9141_ $$y2023
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000588138 915__ $$0LIC:(DE-HGF)CCBY4$$2HGFVOC$$aCreative Commons Attribution CC BY 4.0
000588138 915__ $$0StatID:(DE-HGF)0580$$2StatID$$aPublished
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